This contour integral uses Hankel’s contour Figure 5.9.1.
Assume , collapse the integration path onto the negative real axis,
apply (25.11.25), followed by analytic continuation for all , ,
since the integrand is analytic in , the convergence at the ends of the path is exponential
for all and the Hankel contour can be kept well clear of the singularity at the origin
in the -plane.
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►For the particular loop contour, see Figure 5.9.1.
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§13.23(iii) Hankel Transforms
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►For additional Hankel transforms and also other Bessel transforms see Erdélyi et al. (1954b, §8.18) and Oberhettinger (1972, §1.16 and 3.4.42–46, 4.4.45–47, 5.94–97).
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►For the particular loop contour, see Figure 5.9.1.
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§13.10(v) Hankel Transforms
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►For additional Hankel transforms and also other Bessel transforms see Erdélyi et al. (1954b, §8.18) and Oberhettinger (1972, §§1.16 and 3.4.42–46, 4.4.45–47, 5.94–97).
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L. G. Cabral-Rosetti and M. A. Sanchis-Lozano (2000)Generalized hypergeometric functions and the evaluation of scalar one-loopintegrals in Feynman diagrams.
J. Comput. Appl. Math.115 (1-2), pp. 93–99.